Device for measuring speeds and heat quantities in running media



Ap 7, 1953 N. GLLINDSTROM DEVICE FOR MEASURING SPEEDS AND HEAT QUANTITIES IN RUNNING MEDIA 4 Sheets-Sheet 1 Filed Feb. 5, 1947 I271) 617760.1 JJZ. GILWQZZZ April 7, 1953 N. G. LINDSTRCM 2,633,747

DEVICE FOR MEASURING SPEEDS AND HEAT QUANTITIES IN RUNNING MEDIA Filed Feb. 5, 1947 4 Sheets-Sheet 2 2 I/ F 2 4- 3 I9. 6

l l /ll/ I l 1 E A {k 9 I April 7, 1953 Filed Feb. 5, 1947 N. G. LINDSTRGM DEVICE FOR MEASURING SPEEDS AND HEAT QUANTITIES IN RUNNING MEDIA 4 Sheets-Sheet 3 2(AI-*Bl) April 7, 1953 N. G. LINDSTROM 2,633,747

DEVICE FOR MEASURING SPEEDS AND HEAT QUANTITIES IN RUNNING MEDIA Filed Feb. 5, 1947 4 Sheets-Sheet 4 Patented Apr. 7, 1953 DEVICEFORMEASURING SPEEDS 'ANDHEAT QUANTITIES, IN'RUNNING' MEDIA" Nils Gbttfrid Lindstriim, Stockholm,- Sweden,-;assignorfto' Telefonaktiebclaget' L Bl-r- Ericsson, Stockhoim; -Sweden, a company of. Sweden Application February 5, 1947; Sri'al N 6. 726,606

In'Sweden February 18, 1946 (Ci. 573F193) Claims:v

Tlz'ie present invention relates to anapparatus for m'easuring heatquantities transportedby a running medium or more exactly for measuring the product of the IatGOf-LfiOW" of a-running relation between the --reading of -the measuring... device and the difference of temperature between? two different parts. of. the heat conducting body; .7 in-dcpendenceupon theadifi'erence oi temperature medium and thedifference of-temperature-be 5 between the medium and-saiddevic'eh tween-said'mediumanda.heat -accumulatingdo The curvezI in Fig. .6 is not almear function 1 vice of=any kinds The invention is based on-the A and therefore a measuring device, the readmgof. physical 'law-=thatthe-heat transition constant WhiCh iOllOWS this curve,.1s,-n0t-su1tab1e .t'or. inbetweena-running medium anda heat conducttegraating measurements. Furthermore, the. curve ingbody varies-with'the velocity of themediumyill (10651110511255 through the origin or', coordinates If the said difierence of: temperature -is -constant and thereiore a. constant deduction. must aiways the:velooity-=.of the mediumwill beproportional beemade; Said-iaultscam-however be compen-f to' the'iheamquantity canried by the medium per. sated by. p l neem ms. W ent eeunitoiltimeand to the reading-of themeasuring diumis stationary the omerence cftemperaturef devicai. 16 ttg.tk) :2! is proportionalto the, (inference. of. Accordingto theinvention, a device for mEaSrtemp r v r Q b tw n he m diumnd uring-i-theidifirenc'e of velocityxbetween a run-Te the heat diverting or; heat, emittingldevice. ning, or. gaseous'lmediumzandia wa11 limiting;the1- measuring. (tgtlc) by means-of thermoeiements medium-sis obtained by themediumbeingbrought: and selecting a part, corresponding tothe value 1 toheat orrcoohapart Ofa heatconductingibody. v20 XyOf-theGlBGEIO-HIOHVG Iorce indicating .(to tIO placed onathe same side of the.vvallasthemedium and by connecting the two thermoelements so? and heat insulated. from said wa11,' another part that they counteract each other, it is possible, to of, they r id body 011,.the otherjside.,:ofthe' obtainv anielectr'os-motive force corresponding to" wall: beingjngheat v ;g 11d 1,1c1;ing contact. IWith ta, (tg-.tlC-X). Thus a. relationcorr'espo'nding to heatdiverting lor heat-emitting. device' havinga curveIIl-in Fig. 6 is Obta b tw e reading]? temperatures-differing1from the temperature of. 0 t e measuring device and the. velocity Ofthel the medium, and by a measuring.deviceiprovideda. medium. 7 for measuring; the: (inference F of temperature W measuring e t'q a' t y, integrating? arisingzbymeans;ofthe. deviceebetweenztwo' dif measures or measuresot the average value of the: ierent parts-of: the" heat conductingbody hear" q y Consumption during acertaintimei' Ifthe temperature" fjthe','medi1m1;,.as n are necessary.v By similar measurements "it the temperature 'ofgthe Jheat'. emitting. device :is. desirable that a iinearreiation exist'betw'ejenthef constantyasrelation. isaobtainedbetween the ve reading-0f the rin device "and the heat. locity-of: themediumand the? difference of. temquantityconsumedTperWmit e Thisv perature.: (tg;tlc')a betweenitwosdifierent partslofJ- afihieved y' iconductingjbo'di'es therheat conductingbody; which relation is, il.-: at two pla'ce's'in' the medium; where thevelocity lustratedbyithe-curverlin Fig.6.: An electro 0f h medium different, 01fthe"b0diBS"beiIIg motive -forc9;proporfi0nal w t difference-= difi'erent from each other,"therinoelemer tsthen? temperature -(tgtk). an be obtainedbyimeans being introduced at at least onepoint'iri'eachof oi-thermoelements, and'said electro-motiveforce said the p b n choseniso vthat t e can :loeaimpressed' v upona galvancmeter; the scale electro-motivefol'c; Curve in fifi which arrangedt match t t curve 1 a from said thermoelem'entsywill give a linear rela-- in.Fig..,6 so-that the velocity q ofthemedium can tion between the reading of the-measuring device b read. directly, t. high l t .t and thevelocity of'themedium'; whensubtracte'd asymptotically... approaches a li t g -v f from" the; electro-motiveforce 'represent'ed by-* (tg..tlc the measuring. accuracy thereby decu ve I n F -"6. It" Will appear from the d9 A i g, The mea uflng,.device, t has scription' ofthe' embodiments of' the-f invention" limited measuring range,- the sizelof which can ShOWII'iII -Ba d 9yh0WthiS p lvary,.for exampl'e,.by,1etting,partswith different, The invention will-bedes'cribedmore closely with sizesof'tl'ie, heatvconducting body .comein'to conre erence' the accompanying drawings-Figs: tactwith the running medium. If'the. difference 1-9; oftemperature' between the running mediiim'and Fig. 1 showsthe" main device for m'easuririg'th'e" the heat diverting or heat emitting device is not velocity of ajm'edium. A medium with a certain? constant enough to make asatisfactory measurtemperature to is limited 'by' a wall lyin' which" ing result possible, the variations in difierence of thereis-a bushing"? of heatinsulating material;

tr-nr'iperat'uro can be compensated by cha'nging" the- In said bushing, there" is i a heat-conducti'ri 3 3 arranged so that one part of it is inside the medium and another part is in heat conducting relation with a heat diverting or heat emitting body 2, which has a temperature tic difiering from the temperature of the medium. The body 2 may bea cooling device, a heat plant or a plate with room temperature. In the latter case, however, the heat diverting or heat emitting capacity must be so great, that a sufficient difference of temperature tvtk is maintained. In the heat conducting body 3 there are thermoelements at the points 4 and 5. The temperature at point 5 may correspond to the temperature We of the body 2. The heat diverting or heat emitting body 2 acts as comparative object or reference device. The temperature tg at point 4 will be a function of the velocity of the medium. If the medium is stationary a relatively small difference of temperature (tgt7c) is obtained between the points 4 l and 5, it being here assumed that the temperature at point '5 is tk. If the velocity of the medium is very great, the tem perature to will approach the temperature to of the medium. At points 4 and 5 in Fig. 1 there Y is a thermoelement, the functions of which are connected in series so, that every second point in the series will lie at point 4 and every second at point 5. The difference of electro-motive force between the first and the last thermoelement in the series is measured by'a galvanometer 6, the reading of which indicates the velocity q of the medium. The device according to the description presupposes also that the difference of temperature tvtlc is kept-constant, for example, by regulating the temperature tic either automatically or by hand, or by keeping tic at such a high value, that the variations of to can be neglected.

threaded so that it can be screwed into the tube .as a tube, passes right through both conduits and is welded to the walls of the outlet pipe. The inlet pipe I is made of heat insulating material l at the place, where the tube passes through the pipe. The tube 3 is inwardly threaded and contains a thermoelement 4-5 made according to Fig. 4, Said thermoelement consists of two washers a andb of electrically insulating material, for instance, artificial resin.

The washers a and b are fastened each at one end of a bar 0 and provided with holes 6.

ent metallic materials, have been stretched, twisted, and provided with a lump of solder g at the ends .so that they are held in the holes e, as V shown in Fig. ,5. One of the washers, a, is

3. The other washer, b, turns freely in tube 3, but is closely fitted within the walls of said tube in order to obtain a good heat transmission between the tube and the washer. The tube 3 -'is closed at the end which terminates in theinlet The measurement can however also be made by compensating the difierence of temperature tvtk. For this purpose, there is a double pole switch ii) in Fig. l, by means of which the galvanometer can be connected either to the thermoelement 4-5, as described above, or tea thermo-' element 89, which gives an electro-motive force proportional to the difference of temperature te-sic. The thermoelement 8-9 consists of two groups of junctions 8 and 9, one of which assumes the temperature of the medium, and the other the temperature of the reference device 2. begin with, the electro-motive force of the thermoelement 8-9 is being measured. Then a voltage divider I l is set according to the obtained reading of galvanometer 6. After this, the galvanometer is connected to the voltage divider H, the reading of which will then indicate the velocity of the medium. The diiference of temperature tgtlc will, it is therefore seen, vary proportionally with tv-tlc for each diiferent value of the velocity of the medium.

Fig. 2 shows an application of the invention to measurement of heat quantities in the case in which the heat transporting medium has constant temperature and there is a reference device with equally constant temperature. Such conditions can exist, for instance, in a hot water plant, the hot water thereby being kept at a practically constant temperature and used in a room, the room temperature of which only varies within narrow limits. In Fig. 2, l designates an inlet pipe through which the heat transporting medium is conducted. A bushing 1 within said pipe is: made of heat insulating material. Through this bushing within the walls of said pipe a heat conducting body 3 is inserted. The body 3 is in To R the electro-motive forces from thermoelements pipe by a screw 13 of heat insulating material, for instance, wood. In order that the galvanometer 6 shall. show zero when the medium in the pipe is stationary, there is provided a thermoelement 89, the junctions of which are in heat conducting relationship to the inlet and outlet pipes, which condition is provided for by placing them, respectively, in the walls of the pipes at the points 3 and 9. The. thermoelements 8 and 9 are so connected in the circuit that their electromotive force counteracts the electro-motive force of the thermoelements 45.

The galvanometer 5 indicates theproduct of the velocity of the mediumand the difference of temperature tvtlc.' If the area of the pipe I is taken into account in the constant of the galvanometer, the heat consumption in the heat consuming device is measured as described below.

The relation between the velocity of. the medium in the inlet pipe I and the reading of the galvanometer is indicated by curve I in Fig. 6. The temperature of the medium in the inlet pipe is indicated by to and in the outlet pipe by tic. The

thermoelement 4-5 is responsive to the heat conducted through the tube 3 by part of the difference of temperature tetlc. Said part is indicated by tg-tk, supposing that the unthreaded plate I) of the thermoelement 4-5 assumes the temperature tic. If the medium is stationary;

4-5 and 89 will nullify each other. Each element is therefore supposed to produce a certain.

voltage X according to Fig. 6. When the medium starts to move, the electro-motive force from the thermoelement 89 does not change if the temperatures to and tie remain constant, while the temperature tg increases. The value follows the curve II in Fig. 6 If the lemtiaI-Q',

Between said holes, wires dl and d2, made of differmesa-r2472" bothathermoelementszA- -E.and-i 8-14.: The-differ! ence of temperature X will therefore. beipropore tional to tv.tk,- and therefore tg-Jk-X as well as tg-tkF-wi-lhifOr-each separate value. of q, be proportional to the difference of temperature tv-tl Atlow-velocities of the medium, thatisyi between and the value or liters--peri n1inute': within -.which interval-the curve II in Fig.::6':.can1 be-considered asbeing-approximately linearythe-a temperature tgtkX- "can -be assumed 4 130.; bEL-[Q'gGHOB of temperature -tge-tk'-'.X.'.. In orderpto be;

proportional to-thewelocity of the-imedium, as long as the difference of temperature tv-tk remains constant. If the galvanometer B =isgrad= uated so that it"indicates the velocity of the medium accurately for a. certain-:value. 1 of totlc=T, the following equation is valid for the other values "of the- 'difierence' of temperature -w t]: within the interval g i hmt.. As regards the heat-consumption Qg-it is found to be true that K is'ihere'the. constantofthe. galvanometer inmeasurement of the velocityoi-the-medium, and TK 'isthet constant of'the galvanometer in meant-- ment ofthe heat consumption. The heat? consumption'willfthus, within the interval be proportional to the reading of the :gal'vanometer or. to the electrical current provided by the thermoelements' 4-'5 and8-9.' This makes integrating, measurements possible. This can be done. byreading the galvanometerperiodically; but'the preferred instrument for such measurements is an electrolytic meter. Due to the ther moelement-d-E being threaded in the --tube-3,

the element can beexactlyfitted in its" place so that the reading-"of the galvanometerwill be correct.

For' practical use, a heat quantity --meter according to Fig; 3 canthus not'alwaysbe considered' as satisfactory owingtothe deviation in measuring accuracy caused by the curves Iiand II on Fig. 6 not-being straightlines. In'Fig's. 8- 'and;'9,. however, two different methods; of obrtainingr. thermoelectrical;.:. currentsarev shown; .1 whereinsaid currents are proportional: to-the' heat consumption in .a; device the inlet andout' let pipes of which are accessible for measuring.

In Fig 8 .the inlet pipe I has two forked branches la and lb. Inthe branch lb there is a. constriction IT. by means of whichthe velocity of the heat transporting. medium in thebranch lb is reduced in comparison with its speed in the branch. Ian A... heat conducting .body.3, Zshaped.v

..t b is .threaded Ydirectl throu h. the. as a u e y g 65 'locities. .It isipossible.toiobtain-differentveloeie branches la and. lb, as wellas throughthe. out.-.. let. pipe 2-.1 Thetube-3 is heat insulatedfrom the. branches. la-andlb by means ofbushings l, butis welded to..the.out1et. pip'e.2.. Athermoelement 4-5..is. introduced. .in the. tube .3 as described above-iniconneetion-with Fig. 3, and. anotherthermoeleinent 8-9 compensates ior the differ-. ence;oietemperature x at zero ivelocity of the medium 'Ifhe thermoelements .4-Y-5 and. 8-9- thus develop; in I combination: :a thermoelectric;

6%? current; r; which-.1.- is; :proportionak tot: 'tg-etki-Xi where to ,-dependent uponitheetemperaturebf:

thesme'dium andvits-velocityain the: inlet pipeytlc is; thez'temperaturei of themedimni in the; outlet ablezaccurately" to; balance-- the difference. of: term. perature X by means: of the thermoelementthere is. provided a: voltage; divider l lb, byvmeans on which theadecrease-sof. eleetro-motive 'forcez-from-" 1 5 M the thermoelement' 8--9* is set.-

There is;- furthermore ---another thermoelement.

l 4 4 5 screwed: in the. tube-3.: One: set I 4 of the.

junctions-of thisthermoelementaisplaced in-thatpart ofthe' tubewhich is surrounded. by the me:-*

dium inthe branch*lmand-theother. set of'juncw tions l 5 that part:- of the tube which is :sura

rounded by; the :mediumin thebranchil b.- When the velocity of themedium i510 .these sets of :junc1- tions,=..ofthefthermoelements will assume the same temperature. and due; to-that fact'no elec.-.

trical. current; will be: produced, by them. When the medium is I mo.ving,' -ithe: junctions at l 6- 'have i a higher temperaturev than: the junctions at- 15,

sinceitheavelccityiof the mediumiisgreatenin the:

39 branch. la than. in the.-branch. lb. With high.-

velocity ofthe. medium. the; diiference ofttemperature will again decrease *and .at veryqhigh. velocity, .the.temperatures will lee-equalized. The difference of temperature between the junctions l4- and I 5 WillxfOllOW the curve III: in-Fig. ,6. with variation. of. qr; Bymeans; of: small. displacements of, the junctions. l4 and. l ligand by. means.

of.-a voltagevdivider --lla,"the curve 'III can be given such: a shape; .thatthe; difierence. between:

straight line. through the origin of coordinates, within an interval. q.=0 to q=q2. Since the temperatures-for thejunctions I4 and I5 are determined by .the temperature gradient alongihe. tube. 3, their-:electro-motive force will be: pro- "portional to the diiierence of: temperature tU UC" for everysingle value-of (1.1.

If? the ordinate for the'. curve IIII. is indicated byywe obtain;

By means of, thermoelements 45, l4--l 5., and 8-9 a voltage and-"electrical current is thus obtained, which is proportional to the heat con sumption. By impressing. said-voltage on an electrolytic. meter; the. heat consumption dur.--

ing a certain time can be measured.

Itisobviously notnecessary to. divide the inletpipeinto branches for conducting the heat carrying mediumwith respectively: different veties of; the: medium at. spaced'smeasuring points by' constructing the inlet. pipe-With difierent cross sectional areasin tdifierent parts of the lineyand; arrangingtwo tubes:3,$one-. for the junctions; 4, 5 and l 4, andcone. for the; junction l 5'... ItLis not even-:necessary to-provide'v two; spaced apart measuring points; in:v the: inletxpipe -:wh'ere' the medium. has different .veloei-tieszsbut: it; isiinstea'di.

; possible .toiiintro.duce:.zheat; zconductingzvbodies the form of two" tubes of unequal surface areas or with unequal effects in the inlet pipe and to place in said tubes thermoelements, which produce a combined electro-motive force corresponding to the heat consumption.

An embodiment of such a heat quantity meter is shown in Fig. 9, where l is the inlet pipe and 2' the outlet pipe of a heat consuming or heat emitting apparatus. The inlet pipe has a vertical portion, in which there are three measuring tubes 3, 20 and 24, and within which the heat transporting medium, for instance, water, moves upwardly in order to remove possible air bubbles formed on the measuring tubes. The measuring tubes are moreover rust-proof and smooth ground to avoid corrision and sludge formation, which might changethe heat transition constant between the tubes and the medium. The measuring tubes 3, 20 and 24 are heat insulated from the inlet pipe 1 by means of bushing I, and soldered or welded to the outlet pipe 2. The tube 24 has a smaller outer diameter within the inlet pipe than the tubes 3 and 20, which are identical. There are thermoelements in all the measuring tubes. The thermoelements in the tubes 20 and 24 have twice as many junctions as the thermoelements in the tube 3. The temperature of the medium in the inlet pipe is indicated by to and in the outlet pipe by tic, The temperature of the junction positioned in the measuring tube 3 on the side of the inlet pipe, is indicated by to. The junctions 5, 22, and 26 placed on the side of the outlet pipe are assumed to have the temperature tic.

The measuring tube 3 gives an electro-motive force which is represented by the curve Ai or A2 in Fig. '7, where q is the velocity of the'medium. The curve Al thus corresponds to the difference of temperature tg-tk, when tv.-tlc=T1,

since Al goes asymptotically to the value TI. 1

The curve A2 corresponds to tg-tk at another value of to-tic, that is, T2. A thermoelement 8-9 gives an electro-motive force proportional to tv-tk, of which a part XI or X2 is selected by means of the voltage divider II and is applied so that it counteracts the electromotive force from the measuring tube 3. The value Xi holds when tv-tk=T1, and X2 when tvtk=T2. The measuring tube 20 is identical with the measuring tube 3, as stated above, but its thermoelement has twice as many junctions. Half the value of the electro-motive force obtained from the thermoelement in the measuring tube 20 will thus follow the curve Al, if tv-tk=Tl, and A2, if tvtk= T2 in Fig. '7, halfofthe value of the electro-motive force obtained from the thermoelement 24, on the other side, follows another curve Bl, if tv-tk=T1 and B2, if tv-tic=T2. According to said curves, the difference of temperature tgtk increases with the velocity of the medium more slowly in the measuring tube 24 than in the measuring tube 20, which condition depends upon the relative diameters of the tubes, or the relative eifective heat transmitting surfaces of the tubes within the inlet pipe, this being less for the tube 24 than the corresponding surface for the measuring tube 20. By changing the positions of the thermoelements in the tube and by adjustment of the voltage divider H, it is possible to make the curves BI and B2 intersect the curves Al and A2, respectively. The electro-motive force of the thermoelements 2526 is 2Bl or 2B2 and the curves for BliandB2'are showninFig. I7..IfAl,BI,A2,'and1 B2. indicate the ordinates of the curves for an.

8 arbitrary value of' q, the quantities (are in direct proportion so that,

n13 2 .4 2. and 29.42

at q=0 and q=q2. The idea is now to take the difference Al--Bl and substract it from the curve Bl in order to' obtain a straight line. By subtracting Xl from this line, Cl is obtained accord ing to the following formula:

B1 (A1B1) X1=C'1 This can be rewritten z For this purpose the thermoelements 21-22 and 2526 have twice as many junctions as the thermoelement in tube 3. Assuming that: tvtlc=T1, the thermoelement in tube 3 produces an electro-motive force Al the thermoelement in tube 20 an electro-motive force 2Ai, the thermoelement in tube 24 an electro-motive force 2Bl, and the thermoelement 3-9 an electro-motive force XI.

The thermoelectro-motive forces from the measuring tubes 3, 20 and 24 and the voltage divider H are comiected in series, the electro-- motive forces from the measuring tube 20 and the voltage divider ll thereby being cumulative but counteracting the electro-motive forces from the measuringtubes 3 and 24'. The resulting electro-motive force is connected to an electrolytic meter, which will register the total heat consumption during a measuring period. For each value of the velocity q it therefore holds that;

In order to prevent the measuring tubes from 7 being afiected by external conditions as radiation and heat absorption from surrounding bodies, etc., it maybe suitable to encase the measuring device in a heat insulating casing.

' I claim:

1. In an apparatus measuring the product of the rate of flow of a running medium and the difference of temperature between said medium and a heat diverting device, a Wall; one side of which is in contact with said medium, a heat conducting body extending through said wall, one part of said body being washed by the medium, a piece of heat insulating material surrounding and insulating said body from said wall, another part of said body on; the other side of said wall being in heat conducting relation with said heat diverting device, a first thermoelement having its junctions in thermalcontact with said body and in proximity to the wall and the heat diverting de vice, respectively, and giving an electromotive force proportional to the difference of temperai ture between the positions of the junctions along 93 sa-i-dmheat: conducting body, a second thermoelementihaving ione :junction in heat conducting contactiwithi-asaids mediumaand the other junctionaimheat con'ducting contact with said heat. diverting device and giving anelectromotive force proportional to the difference of temperature between ther'me'dium and? said heat diverting device; said: two thermoelements being connected in 'series and opposing each other and their electromotiveforces balancing each other,'when the mediums-is stationary, and an instrument conmediii-m'inside said walLand another part of said 1 body beinginheat conducting relation with thev mediumirrtheother'of said pipes; a piece of heat insulating. material surrounding and insulating said-.body from'said' Wall, a first thermoelement having -'its:junctions:inthermal. contact with said body'inf. proximity to" the inlet and outlet pipes,

respectively, and giving an electromotive force.

proportional tofthe difference of temperature between the positions ofthe junctions along said heatfconducting body, a second thermoelement having its ljuncti'ons in thermal contact with said inl'etand outlet pipes, respectively, and giving an electromotive forceproportional to the difference oftemperature between themedium in said inlet pipe and the medium'in said outlet pipe, said two thermoelements being connected'in series and opposing each" other and their electrornotive forces balancing each other, whenthe medium is stationary, and aninstrument connected to said two thermoelements'for' indicating the algebraic sum 'of the electromotive forces thereof.

3; In an apparatus for measuring the heat exchangebetwe'en a rumiing medium and a heat exchange unit through which said medium pass-es, an inlet pipe and an outlet pipe conducting said medium to and'from'said unit, one of said pipes having two" parallel branches with one branch having--a constricted'section therein for giving whichis contacted by. the :medium inside said 7 wall and conducting heat between themedium in said pipe andthe other one of said pipes, a piece of .heat insulating: material for each a of said shunts surrounding and. isolating the shunt from said wall. a first thermoelement having its junctions in thermal contact with one of said shunts and in proximity to the inlet and outlet pipes, respectively, and giving an electromotive force proportional to the difference of temperature between 'thepositions of the junctions in said shunt, a second thermoelementhaving one junction in thermal contact with each of "said shunts and improximity'to'the inletpipe and giving an electromotive'fiforce proportionalto the diiference of temperature between-thepositions of the junctionsz inlthe.respeetiveishunts; a third thermoelementifhavin'g 1 onesjunctionf in thermal contact with teach ofifsaid r inietran'd .outlet-pipes and giv ing'eaniieleetromotiveiiforeef-proportional. to the -75"' 10;- difference.oftemperature between the mediumin said inlet pipe and the. medium. .in isaid'outletipipe, saidthree thermoelements being connected inseries, said second and said third thermoelements counteracting said .first thermoelement? and the three ele'ctromotive forces nullifyingeach other when the medium is stationary, and an instrument connecteditorthe three thermoelements. for measuringsthe resultingelectromotive force to, show said heat exchange. W

4. In an apparatus for measuring. the heat ex changebetween a running medium andxa heat exchanging .unit passed by said medium, an. inlet pipe and. an outlet pipe conductingrsaid medium; to. andfr'o'm said'unit, three heat conducting shunts in'theiwall of one of said pipes, each .0f said shunts consistirigof ahea't conducting bodyone-part of which is contacted by,,the medium. inside said wall andconducting heat between-the; medium'in said 'pipe'and the other one of said; pipes, pieces of heat insulating material'for each of said shunts surrounding .and insulating the shunt from said wall, a thermoelement for each" of said bodies having its'l'unctions in thermal; contact with the body and in proximity to the" inlet and outlet pipes. respectively, and ,giving'; an electromotive" force. proportional to; the. dif-'j feren'ce of temperature between the positions .of thejunctionsalong the body, one of said .bodies". having less effective heat transmitting'surfa'ce contact with the'medium than the others, the" thermoelement for'one ofltheotheri two bodies:? giving half the electromotive forceof the thermoelementof thev other one, afourth thermoelement having one junction inlthermal contact with each" of saidinletand outlet pipes and giving an electromotive force proportional to the difference of temperature. between." the medium in' said fe'ed' pipe andthe medium in'said outlet pipe, all of i said thermoelements being connected in series}. said thermoelement 'giving'half the 'electromotive force .and'the thermoelement in said body with lesseffetztive heat transmitting surface being counteractedLby the other two andthe four elec-' tromotive forces nullifying each otherwhen the mediumisstationary, andan instrument connected'to'the four thermoelements for measuring: the resulting electromotive force to show said heat exchange.

5. In an apparatus for measuring the heat consumption of aheat interchange device having an; inlet pipe for conducting a heating medium thereto. and.an. outlet pipe. for conducting the exhaust'.medium'therefrom, a heat conducting, hollow body extending through the inlet pipe,. heat insulating. bushings mounted. in the .wall of said .inlet pipe and surrounding saidbody, said" body being in heat interchange relationship with said outlet pipe, and a thermo-couple havin one' junction. within said. body and within. theinlet pipe and the other junction withinsaid body-and i adjacent the outlet pipe. I

6. In an apparatus for measuring the heat consumption of'a heat interchange device having,an inlet pipe for conducting a heating. medium thereto and'an'outlet pipe for conducting the ex-. haust medium therefrom, a heatconducting hol-.- low body extending'through'the inlet pipe andin: heat interchange relationship with the outlet 1 pipe, heat insulatingbushings'mounted in the wall'cf saidinlet pipe and surrounding said body, and a thermo-couple having one junctionwithin" said body' and withintheinletpipe and'th'e other" junction within said body and. adjacent the-outelet: pipe-, and' acrefe'rence: thermoecouplerhavingr; its juncti'onssrespectively; onithe ewalls softhe melet and outlet pipes and differentially connected in series with the first thermo-couple.

, 7. In an apparatus for measuring the heat consumption of a heat interchange device having an inlet pipe for conducting a heating medium thereto and an outlet pipe for conduct ng the exhaust medium therefrom, a heat conducting hollow body extending throu h the inlet pipe and in heat interchange relationship with the outlet pipe,.heat insulating bushings mounted in the wall of the inlet pipe and surrounding said body, and a thermo-couple comprised by a first disc of electrical insulating material mounted in said body adjacent the outlet pipe, a second disc of electrical insulating material mo nted in said body within the inlet pipe. said therrno-cou le being comprised by pairs of elements of opposite thermo-sensitivity, the alternate junctures between the pairs being mounted respective1y on the insulating discs.

8. In an ap aratus for measuring the product of the rate of flow of a running medium and the change of temperature of said med um passing through a heat exchange unit having an inlet pipe and an outlet pipe, said inlet pipe having two different parts in which the velocity is different', a'heat conducting body pos tioned in the walls of the inlet pipe and extending throu h both of said parts, one part of said body inside said walls being contacted by the medium, pieces of heat insulating material insulating said body from the walls of the inlet pipe, another part of said body outside of said inlet pipe being in thermal contact with the medium in said outlet pipe, a first thermoelement having its junctions in thermal contact with the body in the different parts of the inlet pipe for giving an electromotive force proportional to the difference of temperature between the respective parts of the body in the different parts of the inlet pipe, a second thermoelement having one junction in thermal contact with one part of the body within one part of the inlet pipe and the other junction in thermal contact with another part of the body adjacent the outlet pipe for giving an electromotive force proportional to the diiierence of temperature between said parts of the body in said inlet pipe and in said outlet pipe, respectively, and a third thermoelement having its junctions in thermal contact with the inlet pipe and r the outlet pipe, respectively, for givin an electromotive force proportional to the diflerence of temperature between the medium in the inlet and that in the outlet pipe, said three thermoelements being connected in series, the first and last mentioned thermoelements counteracting the second mentioned thermoelement and the three electromotive' forces balancing each other when the medium is stationary, and. an instrument connected to the three thermoelements for indicating the algebraic sum of the electro-motive forces thereof.

9. In an apparatus for measuring the product of the rate of flow of a running medium and the change of temperature of said medium passing through a heat exchange unit having an inlet pipe. and an outlet pipe, two heat conducting bodies mutually alike and a third heat conducting body with less effective heat transmitting surface than said first two bodies positionedin the wall of said inlet pipe, one part of each of said bodies inside the inlet pipe being contacted by the medium, 'a piece of heat insulating material' insulating each of said bodies from the wall ofv the inlet pipe, another part of each of said bodies outside said inlet pipe being in thermal contact with said outlet pipe, a thermoelement in each of said bodies having one junction in thermal contact with the part of each body within said inlet pipe and the other junction in thermal contact with the other part of each body in thermal contact with the outlet pipe and giving an electro-motive force proportional to the difierence in temperature between the positions oi the junctions in said heat conducting bodies, the thermoelement in one of said. two mutually alike bodies having half as many junctions as the other two thermoelements, an additional thermoelement having its junctions in thermal contact with the inlet and outlet pipes, respectively, and giving an electro-motive force proportional to the difference in temperature between the medium in the inlet pipe and that in, the outlet pipe, all of said thermoelements being connected in series, said thermoelement with half as many junctions and the thermoelement in said heat conducting body with less effective heat transmitting surface being counteracted by the other two thermoelements and the four electromotive forces balancing each other when the medium is stationary, and an instrument connected to said four thermoelements for indicating the algebraic sum of the e1ectromotive forces thereof.

10. In an apparatus for measuring the heat exchange between a running medium and a heat exchange unit through which said medium passes, an inlet pipe and an outlet pipe conducting said medium to and from said heat exchange unit, respectively, said inlet pipe being divided into two parallel branches with one of said branches having a constricted sectiont-herein for imparting to said medium a lesser velocity through the branch having the constricted section therein, two heat conducting shunts extending through the walls of the inlet and outlet pipes, one terminating-in the unconstricted branch and the other in the branch having the constricted section of the inlet pipe, each of said heat conducting shunts consisting of a heat conducting body with parts contacted by the medium inside said walls, heat insulating means surrounding said shunts at the points where same pass through the walls of the inlet pipe, said shunts conducting heat between the medium in said inlet pipe and the medium in said outlet pipe, a firstthermoelement having one junction in thermal contact with the end of the heat conducting shunt within the branch having the constricted section of the inlet pipe and the other junction in thermal contact with the end of the heat conducting shunt within the unconstricted section of the inlet pipe for giving an electro-motive force proportional to the differenceof temperature between the positions of the junctions along said shunts, a second thermoelement having its junctions in one of the respective heat conducting shunts with one junction within the inlet pipe and the other junction within the outlet pipe for giving an electromotive force proportional to the difference of temperature between the positions of the junctions along the shunt, and a third-thermoelement having its junctions in thermal contact with the inlet and outlet pipes, respectively, for giving an electro-motive force proportional to the difference in temperature between the medium in the inlet pipe and the medium in the outlet pipe, said three thermoelements being connected in series with said first and third thermoelements couns 13 teracting said second thermoelement and the three electro-motive forces nullifying each other when the medium is stationary, and an instrument connected to said three thermoelements for measuring the resultant electro-motive force to indicate said heat exchange.

NILS GOTTFRID LINDSIRM.

REFERENCES CITED The following references are of record in the file of this patent:

Number Number 10 40 0,6 17 799,747

14 UNITED STATES PATENTS Name Date Peterson Aug. 30, 1927 Lange Apr. 11, 1933 Wile Apr. 9, 1935 Hulsberg Aug. 3, 1948 FOREIGN PATENTS Country Date Germany Aug. 18, 1924 France Apr. 11, 1936 France Sept. 14, 1936 

